Explicit block encodings of boundary value problems for many-body elliptic operators
1Department of Chemistry, University of California, Berkeley
2Berkeley Quantum Information and Computation Center, University of California, Berkeley
3Department of Chemical and Biomolecular Engineering, University of California, Berkeley
4Yau Mathematical Sciences Center, Tsinghua University
5Center for Theoretical Physics, Massachusetts Institute of Technology
6Simons Institute and Department of Mathematics, University of California, Berkeley
7Chemical Sciences Division, Lawrence Berkeley National Laboratory, Berkeley
| Published: | 2025-06-04, volume 9, page 1764 |
| Editor: | Di Fang |
| Eprint: | arXiv:2407.18347v4 |
| Doi: | https://doi.org/10.22331/q-2025-06-04-1764 |
| Citation: | Quantum 9, 1764 (2025). |
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Abstract
Simulation of physical systems is one of the most promising use cases of future digital quantum computers. In this work we systematically analyze the quantum circuit complexities of block encoding the discretized elliptic operators that arise extensively in numerical simulations for partial differential equations, including high-dimensional instances for many-body simulations. When restricted to rectangular domains with separable boundary conditions, we provide explicit circuits to block encode the many-body Laplacian with separable periodic, Dirichlet, Neumann, and Robin boundary conditions, using standard discretization techniques from low-order finite difference methods. To obtain high-precision, we introduce a scheme based on periodic extensions to solve Dirichlet and Neumann boundary value problems using a high-order finite difference method, with only a constant increase in total circuit depth and subnormalization factor. We then present a scheme to implement block encodings of differential operators acting on more arbitrary domains, inspired by Cartesian immersed boundary methods. We then block encode the many-body convective operator, which describes interacting particles experiencing a force generated by a pair-wise potential given as an inverse power law of the interparticle distance. This work provides concrete recipes that are readily translated into quantum circuits, with depth logarithmic in the total Hilbert space dimension, that block encode operators arising broadly in applications involving the quantum simulation of quantum and classical many-body mechanics.

Featured image: Solutions of the Poisson equation with Dirichlet boundary conditions using the projection method established in this work, showing its ability to find solutions on domains that cannot be expressed as simple tensor products of one-dimensional domains. We provide explicit circuit constructions for these and more general kinds of boundary value problems that can be readily employed for cost estimation and algorithm analysis for applications in quantum computational solutions of classical partial differential equations in a broad range of settings.
Popular summary
Here, we analyze the quantum circuit complexities of block encoding the discretized elliptic operators that arise extensively in numerical simulations for classical PDEs, including high-dimensional instances for many-body simulations. We construct quantum circuit primitives and resource estimations to produce block encodings that encode discretized elliptic operators in a variety of boundary conditions. We further introduce techniques that implement these operators using periodic extensions to obtain high-precision approximations, as well as techniques for implementing them on irregular domains. We then present a scheme to efficiently block encode the many-body convective operator for particles interacting by a pair-wise potential, opening a route to efficient quantum algorithms to simulate high-dimensional Fokker-Planck and Smoluchowski-type equations for many-body systems.
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